Unit 5: Rotational Motion
5.1: Rotational Kinematics
Introduction
Rotational kinematics describes motion around a fixed axis. It is analogous to linear kinematics, but instead of displacement, velocity, and acceleration, we use **angular displacement (θ), angular velocity (ω),** and **angular acceleration (α).**
Key Concepts
- Angular Displacement (θ): Measured in radians, represents the change in rotational position.
- Angular Velocity (ω): The rate of change of angular displacement (rad/s).
- Angular Acceleration (α): The rate of change of angular velocity (rad/s²).
- Direction: Counterclockwise is usually positive; clockwise is negative.
Mathematical Routines
- Angular kinematic equations (analogous to linear kinematics):
- ω = ω₀ + αt
- θ = ω₀t + ½ αt²
- ω² = ω₀² + 2αθ
- Radians as the natural unit for angular displacement.
- Converting between degrees and radians: \(1 \text{ rad} = 57.3^\circ\).
Tip: Use the same approach for solving rotational problems as linear kinematics—list known values, choose the right equation, solve algebraically, and check units.
Creating Representations
- Diagrams: Use circular motion diagrams with labeled angular displacement, velocity, and acceleration.
- Graphs: Plot θ vs. t, ω vs. t, and α vs. t to analyze motion.
Scientific Questioning & Argumentation
- Question: "What happens when α is zero?"
- Argumentation: No angular acceleration means constant ω, similar to constant velocity in linear motion.
Practice Activities
Activity 1: Calculating Angular Displacement
A wheel starts from rest and accelerates at 2 rad/s² for 4 seconds. Find its angular displacement.
Summary & Exam Preparation Tips
- Use kinematic equations for angular motion just like in linear motion.
- Pay attention to sign conventions (counterclockwise = positive).